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EntityQ1043902· pop 31· linked from 497 articles

galaxy

Astronomical data · SIMBAD

Object type
AG?
Redshift
z = 0.008206
Morphology
SBb
Coordinates
RA 65.8629° · Dec 75.2956°
View on SIMBAD →

via SIMBAD · CDS Strasbourg

Key facts

Constellation
Camelopardalis
Right ascension
04 23 27.102
Declination
+75 ° 17 ′ 44.05 ″
Redshift
0.008209 ± 0.000013
Heliocentric radial velocity
2,459 km/s
Galactocentric velocity
2,622 km/s
Distance
65 Mly (19.9 Mpc )
Type
SB(rs)bc
Apparent size v
4.6 ′ × 2.4 ′

via Wikipedia infobox

Wikidata facts

Distance from Earth
18
Image
N1530s-crop.jpg
Show 9 more facts
catalog code
LEDA 15018
Commons category
NGC 1530
time of discovery or invention
1877-00-00
redshift
0.008209
apparent magnitude
8.285
galaxy morphological type
SBb
right ascension
65.8629250
declination
75.2955694
radial velocity
2450

via Wikidata · CC0

~5 min read

Article

NGC 1530 is a barred spiral galaxy in the northern constellation of Camelopardalis. It was discovered by German astronomer W. Tempel in 1876. Danish astronomer J. L. E. Dreyer in 1888 described it only as large and pretty bright. NGC 1530 has an apparent visual magnitude of 12.3 and an angular size of 4.6′ × 2.4′. The plane of the galactic disk is inclined at an angle of 55° to the line of sight from the Earth. This galaxy is located at an estimated distance of 65 million light years, with a recessional velocity of 2,622 km/s relative to the Milky Way galaxy. It is a relatively isolated galaxy with its nearest neighbor being NGC 1530A at an angular separation of 19′.

HST partial image of NGC 1530 showing the central region and part of the bar NGC 1530 has a morphological classification of type SB(rs)bc in the de Vaucouleurs system, which means it is a barred spiral galaxy (SB) with a transitional outer ring structure (rs) that joins somewhat loosely wound arms (bc). The bar structure in this galaxy is unusually large and strong, spanning an angular size of 100″. It includes a clumpy, star-forming nuclear ring structure with a radius of 21″. Star formation is particularly high in the nucleus region and at the ends of the bar, but weak in between these locations. This activity appears to be taking place primarily on the trailing side of the bar where gas pressure is highest. Two linear dust lanes are visible along the bar, which outline shock fronts in the flow of gas.

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